Reflection and Refraction, much index of refraction

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SUMMARY

The critical angle for a glass-water interface is calculated using Snell's Law, specifically the formula θcrit = sin-1(n2/n1). With the refractive indices of water (n2 = 1.33) and glass (n1 = 1.50), the critical angle is determined to be approximately 62.46 degrees. Total internal reflection occurs when light travels from a denser medium (glass) to a less dense medium (water). The discussion clarifies the correct application of Snell's Law and emphasizes the importance of accurate calculations to avoid invalid results.

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  • Understanding of Snell's Law in optics
  • Knowledge of refractive indices (e.g., water and glass)
  • Ability to perform inverse sine calculations
  • Familiarity with the concept of total internal reflection
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  • Explore the concept of total internal reflection in optical fibers
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Homework Statement


1. The index of refraction for water is 1.33 and that of glass is 1.50.

a. What is the critical angle for a glass-water interface?b. In which medium is the light ray incident for total internal reflection?

Homework Equations


nisin\varthetai=nrsin\varthetar

The Attempt at a Solution


a. I think the answer to a. is 62.46 degrees, but I am not sure.
b. I think the answer is glass, simply because it is going to be moving from a less dense area to a more dense area.
 
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Use Snell's law:

n_1\sin\theta_1 = n_2\sin\theta_2\ .

Note: It's not additive like you suggested.

At the critical angle, \theta_2 is 90 degrees (the light refracts along the boundary). That is to say, it's sin is 1. We can therefore rearrange for the critical angle:

\theta_{\mathrm{crit}} = \sin^{-1} \left( \frac{n_2}{n_1} \right)

Now we have two refractive indices, the glass and the water. If you plug them in incorrectly, you're going to end up with trying to find the inverse sin of a value > 1, which isn't possible as this has no solution.
 
astrorob said:
Use Snell's law:

n_1\sin\theta_1 = n_2\sin\theta_2\ .

Note: It's not additive like you suggested.

At the critical angle, \theta_2 is 90 degrees (the light refracts along the boundary). That is to say, it's sin is 1. We can therefore rearrange for the critical angle:

\theta_{\mathrm{crit}} = \sin^{-1} \left( \frac{n_2}{n_1} \right)

Now we have two refractive indices, the glass and the water. If you plug them in incorrectly, you're going to end up with trying to find the inverse sin of a value > 1, which isn't possible as this has no solution.

Quite sorry for the mistake in Snell's Law. I knew what it meant, I just messed up when writing it in the forum.

Anyway, I appreciate the input, but if you are using
\theta_{\mathrm{crit}} = \sin^{-1} \left( \frac{n_2}{n_1} \right), would it not be possible to put 1.33 (n2) over 1.5 (n1)? This would look like
\theta_{\mathrm{crit}} = \sin^{-1} \left( \frac{1.33}{1.5} \right) and if plugged into a calculator, would return 62.45732485 degrees.
 
For this problem I calculated 62.4 degrees, the same thing you got.

As for B, I put water.
 
Yes, that's correct as you've stated.

It also gives you the answer to your second question as n_2 represents the refractive index of the medium that the light traveling in medium n_1 is incident on.
 
patriots1049 said:
For this problem I calculated 62.4 degrees, the same thing you got.

As for B, I put water.

Ah, thank you. I was actually thinking that it would be glass because my book details the fact that "Total internal reflection occurs when light passes from a more optically dense medium to a less optically dense medium at an angle so great that there is no refracted ray." This would mean that glass-water would be a more optically dense to a less optically dense scenario.
 
astrorob said:
Yes, that's correct as you've stated.

It also gives you the answer to your second question as n_2 represents the refractive index of the medium that the light traveling in medium n_1 is incident on.

Thank you very much. You have been a big help today, astrorob.
 

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